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Let 9 v=9v +g be an infinitesimal deformation of the metric tensor. Demon- strate that the Christoffel symbols Ip and the Riemann tensor Ro

Let gw- gaw-guv + ?3pv be an infinitesimal deformation of the metric tensor. Demon- strate that the Christoffel symbols i ??? and the Riemann tensor R0?? change as follows Additional problem for Daniel, Emmanouil, James and Michael Given a d-dimensional spacetime, consider a Weyl transformation of the metric tensor, guv ? ???-e2gw, with ? and arbitrary smooth function. (a) Compute the Weyl-transformed Riemann tensor ?.??. (b) Consider the Weyl tensor defined by where 2 2(d-1) is the so-called Schouten tensor. Demonstrate that Weyl tensor CP ou is invariant under the Weyl transformation. (c) Demonstrate that the Weyl tensor (i) has all the algebraic properties of the Riemann tensor; and (ii) it is traceless ?pu

Let 9 v=9v +g be an infinitesimal deformation of the metric tensor. Demon- strate that the Christoffel symbols Ip and the Riemann tensor Ro change as follows: vp ST" = vp where 1 59 {V89= +V89v -V489,p) , SR = Vvo - V. Additional problem for Daniel, Emmanouil, James and Michael Given a d-dimensional spacetime, consider a Weyl transformation of the metric tensor, 9v = 0 , with o and arbitrary smooth function. (a) Compute the Weyl-transformed Riemann tensor Rgv. (b) Consider the Weyl tensor defined by po = Rp 9pu Pov + go Ppv +9pv Po - gov Ppp, Pv 1 (Rp 2(d - 179R) 1 d = 2 (Ruv d-2 is the so-called Schouten tensor. Demonstrate that Weyl tensor Co is invariant under the Weyl transformation. (c) Demonstrate that the Weyl tensor (i) has all the algebraic properties of the Riemann tensor; and (ii) it is traceless, CP apv=0.

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